1. CROSS SECTIONAL AREA (A): The
cross sectional area expressed in square inches is used in various
tubular goods equations. The formulas described below are based on
full sections, exclusive of corner radii.
{1a} Round Tube: A = p/4 (D5 -
d5)
Where:
D = Outside Diameter, inches d = Inside Diameter,
inches
Example: Calculate the cross sectional area of a 7"
O.D. x .500" wall tube.
D = 7.000 d = 7.000 - 2(.500) = 6.000 inches
A = p/4 (D5 - d5)
A = 3.1415/4 (7.0005 - 6.0005)
A = 10.210 inches
{1b} Square Tube: A = D5 - d5
Where:
D = Outside Length, inches d = Inside Length, inches
Example: Calculate the cross sectional area of a 7"
O.D. x .500" wall tube.
D = 7.000 d = 7.000 - 2(.500) = 6.000 inches
A = D5 - d5
A = 49 - 36 = 13
A = 13.00 inches5
{1c} Rectangular Tube: A = D1D -
d1d
Where:
D = Outside Length, long side, inches
D1= Outside Length, short side, inches
d = Inside Length, long side, inches
d1= Inside Length, short side, inches
Example: Calculate the cross sectional area of a
4" x 6" rectangular tube with .500"
wall thickness.
D = 6.00" D1= 4.00" d = 5.00"
d1= 3.00"
A = D1D - d1d
A = 4.00 (6.00) - 3.00 (5.00) = 9.00
A = 9.00 inches5
2. PLAIN END WEIGHT (Wpe):The
plain end weight expressed in pounds per foot is used in connection
with pipe to describe the nominal or specified weight per foot. This
weight does not account for adjustments in weight due to end finishing
such as upsetting or threading.
{2} Wpe = 10.68 (D - t)t
Where:
Wpe = plain end weight, calculated to 4
decimal places and rounded to 2 decimals, pounds/foot
D = Specified Outside Diameter of the Pipe, inches
t = Specified Wall Thickness, inches
Example: Calculate the plain end weight of pipe
having a specified O.D. of 7 inches and a wall thickness of .540
inches.
Wpe = 10.68 (7.000 - .540) .540
Wpe = 37.2561
Wpe = 37.26 pounds/foot
3. INTERNAL YIELD PRESSURE BURST-RESISTANCE (P):
The internal yield pressure or burst resistance of
pressure bearing pipe is expressed in pounds/square inch (psi). The
.875 factor is to allow for minimum permissible wall based on API
criteria for OCTG and line pipe. This factor can be changed based on
other applicable specifications regarding minimum permissible wall
thickness.
{3} P = 0.875 [ 2 Yp t/D]
Where:
P = Minimum Internal Yield Pressure (Burst
Resistance) in pounds per square inch, rounded to the nearest 10 psi.
Yp= Specified Minimum Yield Strength,
pounds per square inch.
t = Nominal (specified) Wall Thickness, inches
D = Nominal (specified) Outside Diameter, inches
Example: Calculate the burst resistance of 7"
O.D. x .540" wall API L80 casing.
P = 0.875 [ 2 Yp t/D]
P = 0.875 [ (2)(80,000)(.540)/7]
P = 10,800 psi
4. PIPE SPECIFICATIONS BASICS
Pressure Determinations:Barlow's Formula is
commonly used to determine:
1. Internal Pressure at Minimum Yield
2. Ultimate Bursting Pressure
3. Maximum Allowable Working Pressure
4. Mill Hydrostatic Test Pressure
This formula is expressed as P = 2St where:
P = Pressure, psig
I = Nominal wall thickness, inches
D = Outside Diameter, inches
S = Allowable Stress, psi, which depends on the
pressure being determined
To illustrate, assume a piping systems 8 5/8"
O.D. x .375" wall has a specified minimum yield strength (SMYS)
of 35,000 psi and a specified minimum tensile strength of 80,000 psi.
For 1. Internal Pressure of Minimum Yield
S = SMYS (35,000) psi and
P = 2St = (2)(35,000)(0.375)
D 8.625 = 3043 or 3040 psig (rounded to nearest 10
psig)
For 2. Ultimate Bursting Pressure
S = Specified Minimum Tensite Strength (60,000 psi)
and
P = 2St = (2)(60,000)(0.375)
D 8.625 = 5217 or 5220 psig (rounded to nearest 10
psig)
For 3. Maximum Allowable Working Pressure
(MAOP)
S = SMYS (35,000 psi) reduced by a design factor,
usually 0.72 and
P = 2St = (2)(35,000 x 2)(0.375)
D 8.625 = 2191 or 2190 psig (rounded to nearest 10
psig)
For 4. Mill Hydrostatic Test Pressure
S = SMYS (35,000 psi) reduced by a factor depending
on O.D. grade (0.60 for 8 5/8" O.D. grade B) and
P = 2St = (2)(35,000 x 0.60)(0.375)
D 8.625 = 1826 or 1830 psig (rounded to nearest 10
psig)
Wall Thickness
Barlow's Formula is also useful in determining the
wall thickness required for a piping system. To illustrate, assume a
piping system has been designed with the following criteria:
1. A working pressure of 2,000 psi (P)
2. The pipe to be used is 8 5/8" O.D. (D)
specified to ASTM A53 grade B (SMYS - 35,000 psi)
Rearranging Barlow's Formula to solve for wall
thickness gives:
t = PD = (2,000) (8.625) = 0.246"
wall
2S (2) (35,000)
Wall thickness has no relation to outside diameter -
only the inside diameter is affected. For example, the outside
diameter of a one-inch extra- strong piece of pipe compared with a
one-inch standard weight piece of pipe is identical; however, the
inside diameter of the extra-strong is smaller than the inside
diameter of the standard weight because the wall thickness is greater
in the extra-strong pipe.
5. WATER DISCHARGE MEASUREMENTS: To
calculate the volume being displaced through a pipe or the amount of
volume of an irrigation well, the following formula is applicable:
Q = 3.61 A H %Y
Where:
Q = Discharge in Gallons per minutes
A = Area of the pipe, inches squared
H = Horizontal measurement, inches
Y = vertical measurement, inches
Example:Calculate the discharge of a 10" pipe
which has an area of 78.50 in2, a horizontal measurement
of 12" and a vertical measurement of 12".
Q = 3.61 A H
%Y
Q = 3.61 (78.50) (12)
%12
Q = 3400.62
3.464
Q = 981.70 gallons per minute
This formula is a close approximation of the actual
measurement of the volume being displaced. The simplest method is to
measure a 12 inch vertical measurement as a standard procedure, then
measure the distance horizontally to the point of the 12"
vertical measurement.
GENERAL TECHNICAL INFORMATION
WATER
One miner's inch: 1 1/2 cubic feet per minute =
11.25 U.S. gallons per minute = flow per minute through 1 inch square
opening in 2 inch thick plank under a head of 6 1/2 inches to center
of orifice in Arizona, California, Montana, Nevada and Oregon. 9 U.S.
gallons per minute in Idaho, Kansas, Nebraska, New Mexico, North
Dakota, South Dakota and Utah.
One horse-power: 33,000 ft. pounds per minute
Cubic feet per second:Gallons per minute 449
Theoretical water US GPM x head in feet x Sp. Gr.
horse-power: 3960
Theoretical waterUS GPM x head in pounds
horse-power: 1714
Brake horse-power:Theoretical water horse-power
Pump efficiency
Velocity in feet.408 x US Gal Per Min = .32
x GPM
per second: Pipe diameter in inches2
pipe area
One acre-foot: 325,850 US gallons
1,000,000 US gallons per day: 695 US gallons per
minute
500 pounds per hour: 1 US gallon per minute
Doubling the diameter of a pipe or cylinder
increases its capacity four times
Friction of liquids in pipes increases as the square
of the velocity.
Velocity in feet per minute necessary to discharge a
given volume of water, in a given time =
Cubic Feet of water x 144
area of pipe in sq. inches
Area of required pipe, the volume and velocity of
water being given = No. cubic feet water x 144
Velocity in feet per min.
From this area the size pipe required may be
selected from the table of standard pipe dimensions.
Atmospheric pressure at sea level is 14.7 pounds per
square inch. This pressure with a perfect vacuum will maintain a
column of mercury 29.9 inches or a column of water 33.9 feet high.
This is the theoretical distance that water manu be drawn by suction.
In practice, however, pumps should not have a total dynamic suction
lift greater that 25 feet.
CRUDE OIL
One gallon: 58,310 grains
One barrel oil: 42 US gallons
One barrel per hour: .7 US gallons per minute
Gallons per minute: bbls. per day x .02917
Bbls. per hour: gallons per minute x .7
One barrel per day: .02917 gallons per minute
Gallons per minute: bbls. per day x .02917
Bbls. per day: gallons per minute x .02917
Velocity in feet per second: .0119 x bbls. per day x
pipe dia. in inches2 x .2856 x bbls. per hour x pipe dia.
in inches2
Net horse-power: The theoretical horse-power
necessary to do the work
Net horse-power: Barrels per day x pressure x
.000017
Net horse-power: Barrels per hour x pressure x
.000408
Net horse-power: Gallons per min. x pressure x
.000583
The customary method of indicating specific gravity
of petroleum oils in this country is by means of the Baume scale.
Since the Baume scale, for specific gravities of liquids lighter than
water, increases inversely as the true gravity, the heaviest oil,
i.e., that which has the highest true specific gravity, is expressed
by the lowest figure of the Baume scale; the lightest by the highest
figure.
MISCELLANEOUS
Areas of circles are to each other as the squares of
their diameters.
Circumference diameter of circle x 3.1416
Area circle diameter squared x .7854
Diameter circle circumference x .31831
Volume of sphere cube of diameter x .5236
Square feet square inches x .00695
Cubic feet cubic inches x .00058
Cubic yard cubic feet x .03704
Statute miles lineal feet x .00019
Statute miles lineal yards x .000568
1 gallon 8.33 pounds
1 liter .2642 gallons
1 cubic feet 7.48 gallons and/or 62.35 pounds
1 meter 3.28 feet
STATIC HEAD
Static head is the vertical distance between the
free level of the source of supply and the point of free discharge, or
to the level of the free surface of the discharged liquid.
TOTAL DYNAMIC HEAD
Total dynamic head is the vertical distance between
source of supply and point of discharge when pumping at required
capacity, plus velocity head friction, entrance and exit losses.
Total dynamic head as determined on test where
suction lift exists, is the reading of the mercury column connected to
the suction nozzle of the pump, plus reading of a pressure gage
connected to discharge nozzle of pump, plus vertical distance between
point of attachment of mercury column and center of gage, plus excess,
if any, of velocity head of discharge over velocity head of suction,
as measured at points where the instruments are attached, plus head of
water resting on mercury column, if any.
Total dynamic head, as determined on tests where
suction head exists, is the reading of the gage attached to the
discharge nozzle of pump, minus the reading of a gage connected to the
suction nozzle of pump, plus or minus vertical distance between
centers of gages (depending upon whether suction gage is below or
above discharge gage), plus excess, if any, of the velocity head of
discharge over velocity head of suction as measured at points where
instruments are attached.
Total dynamic discharge head is the total dynamic
head minus dynamic suction lift, of plus dynamic suction head.
SUCTION LIFT
Suction lift exists when the suction measured at the
pump nozzle and corrected to the centerline of the pump is below
atmospheric pressure.
Static suction lift is the vertical distance from
the free level of the source of supply to centerline of pump.
Dynamic suction lift is the vertical distance from
the source of supply when pumping at required capacity, to centerline
of pump, plus velocity head, entrance and friction loss, but not
including internal pump losses, where static suction head exists but
where the losses exceed the static suction head the dynamic suction
lift is the sum of the velocity head, entrance, friction, minus the
static suction head, but not including internal pump losses.
Dynamic suction lift as determined on test, is the
reading of the mercury column connected to suction nozzle of pump,
plus vertical distance between point of attachment of mercury column
to centerline of pump, plus bead of water resting on mercury column,
if any.
SUCTION HEAD
Suction head (sometimes called head of suction)
exists when the pressure measured at the suction nozzle and corrected
to the centerline of the pump is above atmospheric pressure.
Static suction head is the vertical distance from
the free level of the source of supply to centerline of pump.
Dynamic suction head is the vertical distance from
the source of supply, when pumping at required capacity, to centerline
of pump, minus velocity head, entrance, friction, but not minus
internal pump losses.
Dynamic suction head, as determined on test, is the
reading of a gage connected to suction nozzle of pump, minus vertical
distance from center of gage to center line of pump. Suction head,
after deducting the various losses, many be a negative quantity, in
which case a condition equivalent to suction lift will prevail.
VELOCITY HEAD
The velocity head (sometimes called "head due
to velocity") of water moving with a given velocity, is the
equivalent head through which it would have to fall to acquire the
same velocity: or the head necessary merely to accelerate the water.
Knowing the velocity, we can readily figure the velocity head from the
simple formula:
h = V2
2g
in which "g" is acceleration due to
gravity, or 32.16 feet per second; or knowing the head, we can
transpose the formula to:
V = %2 gh
and thus obtain the velocity.
The velocity head is a factor in figuring the total
dynamic head, but the value is usually small, and in most cases
negligible; however, it should be considered when the total head is
low and also when the suction lift is high.
Where the suction and discharge pipes are the same
size, it is only necessary to include in the total head the velocity
head generated in the suction piping. If the discharge piping is of
different size than the suction piping, which is often the case, then
it will be necessary to use the velocity in the discharge pipe for
computing the velocity head rather than the velocity in the suction
pipe.
Velocity head should be considered in accurate
testing also, as it is part of the total dynamic head and consequently
affects the duty accomplished.
In testing a pump, a vacuum gage or a mercury column
is generally used for obtained dynamic suction lift. The mercury
column or vacuum gage will show the velocity head combined with
entrance head, friction head, and static suction lift. On the
discharge side, a pressure gage is usually used, but a pressure gage
will not indicate velocity head and this must, therefore, be obtained
either by calculating the velocity or taking reading with a Pitometer.
Inasmuch as the velocity varies considerably at different points in
the cross section of a stream it is important, in using the Pitometer,
to take a number of readings at different points in the cross section.
A table, giving the relation between velocity and
velocity head is printed below:
| Velocity
in feet per second |
Velocity
head in feet |
Velocity
in feet per second |
Velocity
head in feet |
| 1 |
.02 |
9.5 |
1.40 |
| 2 |
.06 |
10 |
1.55 |
| 3 |
.14 |
10.5 |
1.70 |
| 4 |
.25 |
11 |
1.87 |
| 5 |
.39 |
11.5 |
2.05 |
| 6 |
.56 |
12 |
2.24 |
| 7 |
.76 |
13 |
2.62 |
| 8 |
1.00 |
14 |
3.05 |
| 8.5 |
1.12 |
15 |
3.50 |
| 9 |
1.25 |
|
|
NET POSITIVE SUCTION HEAD
NPSH stands for "Net Positive Suction Head".
It is defined as the suction gage reading in feet absolute taken on
the suction nozzle corrected to pump centerline, minus the vapor
pressure in feet absolute corresponding to the temperature of the
liquid, plus velocity head at this point. When boiling liquids are
being pumped from a closed vessel NPSH is the static liquid head in
the vessel above the pump centerline minus entrance and friction
losses.
VISCOSITY
Viscosity is the internal friction of a liquid
tending to reduce flow.
Viscosity is ascertained by an instrument termed a
Viscosimeter, of which there are several makes, viz. Saybolt
Universal; Tangliabue; Engler (used chiefly in Continental countries);
Redwood (used in British Isles and Colonies). In the United States the
Saybolt and Tangliabue instruments are in general use. With few
exceptions. Viscosity is expressed as the number of seconds required
for a definite volume of fluid under a arbitrary head to flow through
a standardized aperture at constant temperature.
SPECIFIC GRAVITY
Specific gravity is the ratio of the weight of any
volume to the weight of an equal volume of some other substance taken
as a standard at stated temperatures. For solids or liquids, the
standard is usually water, and for gasses the standard is air or
hydrogen.
Foot pounds: Unit of work
Horse Power (H.P.): (33,000 ft. pounds per minute -
746 watts - .746 kilowatts) Unit for measurement of power or rate of
work
Volt-amperes: Product of volts and amperes
Kilovolt-Amperes (KVA): 1000 volt-amperes
Watt-hour: Small unit of electrical work - watts
times hours
Kilowatt-hour (KWHr): Large unit of electrical work
- 1000 watt-hours
Horse Power-hour (HPHr): Unit of mechanical work
To determine the cost of power, for any specific
period of time - working hours per day, week, month or year:
No. of working hrs, x .746 x H.P. motor = KWHr
consumed
Efficiency of motor at Motor Terminal
KWHr consumed at Motor Terminal x Rate per KWHr =
Total cost current for time specified
Torque is that force which produces or tends to
produce torsion (around an axis). Turning effort. It may be thought of
as a twist applied to turn a shaft. It can be defined as the push or
pull in pounds, along an imaginary circle of one foot radius which
surrounds the shaft, or, in an electric motor, as the pull or drag at
the surface of the armature multiplied by the radius of the armature,
the term being usually expressed in foot-pounds (or pounds at 1 foot
radius).
Starting torque is the torque which a motor exerts
when starting. It can be measured directly by fastening a piece of
belt to 24" diameter pulley, wrapping it part way round and
measuring the pounds pull the motor can exert, with a spring balance.
In practice, any pulley can be used for torque = lbs. pull x pulley
radius in feet. A motor that has a heavy starting torque is one that
starts up easily with a heavy load.
Running torque is the pull in pounds a motor exerts
on a belt running over a pulley 24" in diameter.
Full load torque is the turning moment required to
develop normal horse-power output at normal speed.
The torque of any motor at any output with a known
speed may be determined by the formula:
T = Brake H.P. x 5250
R.P.M.
With a known foot-pounds torque, the horse-power at
any given speed can be determined by the formula:
H.P. = T x R.P.M.
5250
H.P. = T x speed of belt on 24"pulley in feet
per minute 33000
COST OF PUMPING WATER
Cost per 1000 gallons pumped: .189 x power cost per
KWHr x head in feet
Pump eff. x Motor eff. x 60
Example: Power costs .01 per k.w.-hour; pump
efficiency is 75%; motor efficiency is 85%; total head is 50 feet.
.189 x .01 x 50 = $ .0025 or 1/4 of a cent
.75 x .85 x 60
Cost per hour of pumping:
.000189 x g.p.m. x head in ft x power cost per KWHr
Pump efficiency x Motor efficiency
Cost per acre foot of water:
1.032 x head in ft x power per KWHr
Pump efficiency x Motor efficiency
Pump efficiency: g.p.m. x head in feet
3960 x b.h.p. (to pump)
Head: 3960 x Pump eff. x b.h.p x g.p.m.
b.h.p. (Brake horse-power) to pump: Motor efficiency
x h.p. at motor
b.h.p.: g.p.m. x head in feet x 3960 x Pump eff.
g.p.m.: 3960 x Pump eff. x b.h.p. x head in feet
COMPUTING H.P. INPUT FROM REVOLVING WATT HOUR
METERS
(Disk Constant Method)
Kilowatts Input = KW in = K x R x 3.60 x t
HP Input = HP in = K x R x 3600 = 4.83 x K x R x t x
746 t
K - constant representing number os watt-hours
through meter for on revolution of the disk. (Usually found on meter
nameplate or face of disk)
R - number of revolutions of the disk
t - seconds for R revolutions
Cost per 1000 gallons of water:
C = 746 x r x HP in x GPH
C - cost in dollars per 1000 gallons
r - power rate per kilowatt hour (dollars)
HP in - HP input measured at the meter (see above)
H - total pumping head
GPH - gallons per hour discharged by pump
Cost per 1000 gallons of water
For each foot of head:
C = 746 x r x HP in x H x GPH
Cost per hour:
C = .746 x r x HP in